warm up - city university of new york

102
Warm up Recall, to graph a conic function, you want it in the form parabola: (x - x 0 ) 2 =4p(y - y 0 ) or (y - y 0 ) 2 =4p(x - x 0 ), ellipse: ( x-x 0 a ) 2 + ( y-y 0 b ) 2 =1, hyperbola: ( x-x 0 a ) 2 - ( y-y 0 b ) 2 =1 or ( y-y 0 a ) 2 - ( x-x 0 b ) 2 =1 Without doing any algebraic manipulation, decide whether each of the following conic sections is a parabola, ellipse, or hyperbola. Can you tell which way it’s oriented? 1. 36y 2 - x 2 + 72y +6x + 31 = 0 2. y 2 - 10y - 8x + 49 = 0 3. y 2 +2x 2 +4y +8x + 11 = 0 Now, complete squares and put into a form you can graph from. Identify (as applicable) the vertices, foci, axes, directrixes, asymptotes.

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Page 1: Warm up - City University of New York

Warm up

Recall, to graph a conic function, you want it in the formparabola: (x− x0)2 = 4p(y − y0) or (y − y0)2 = 4p(x− x0),

ellipse:(x−x0a

)2+(y−y0

b

)2= 1,

hyperbola:(x−x0a

)2 − (y−y0b

)2= 1 or

(y−y0a

)2 − (x−x0b

)2= 1

Without doing any algebraic manipulation, decide whether each ofthe following conic sections is a parabola, ellipse, or hyperbola.Can you tell which way it’s oriented?

1. 36y2 − x2 + 72y + 6x+ 31 = 0

(x−32

)2 − (y+11/3

)2= 1

2. y2 − 10y − 8x+ 49 = 0

(y − 5)2 = 4(2)(x− 3)

3. y2 + 2x2 + 4y + 8x+ 11 = 0

(y + 2)2 +(

x+21/√2

)2= 1

Now, complete squares and put into a form you can graph from.Identify (as applicable) the vertices, foci, axes, directrixes,asymptotes.

Page 2: Warm up - City University of New York

Warm up

Recall, to graph a conic function, you want it in the formparabola: (x− x0)2 = 4p(y − y0) or (y − y0)2 = 4p(x− x0),

ellipse:(x−x0a

)2+(y−y0

b

)2= 1,

hyperbola:(x−x0a

)2 − (y−y0b

)2= 1 or

(y−y0a

)2 − (x−x0b

)2= 1

Without doing any algebraic manipulation, decide whether each ofthe following conic sections is a parabola, ellipse, or hyperbola.Can you tell which way it’s oriented?

1. 36y2 − x2 + 72y + 6x+ 31 = 0(x−32

)2 − (y+11/3

)2= 1

2. y2 − 10y − 8x+ 49 = 0 (y − 5)2 = 4(2)(x− 3)

3. y2 + 2x2 + 4y + 8x+ 11 = 0 (y + 2)2 +(

x+21/√2

)2= 1

Now, complete squares and put into a form you can graph from.Identify (as applicable) the vertices, foci, axes, directrixes,asymptotes.

Page 3: Warm up - City University of New York

36y2 − x2 + 72y + 6x+ 31 = 0: Hyperbola!

0 = 36y2−x2 + 72y + 6x+ 31

= 36(y2 + 2y)− (x2 − 6x) + 31

= 36((y + 1)2 − 1)− ((x− 3)2 − 9) + 31

= 36(y + 1)2 − (x− 3)2 + 4.

So 4 = (x− 3)2 − 36(y + 1)2. So

1 = (x− 3)2/4− 9(y + 1)2 =(x−32

)2 − (y+11/3

)2.

center: (3,−1); a = 2, b = 1/3,c =

√22 + (1/3)2 =

√37/3 ≈ 2.03; ;

vertices: (3± 2,−1);foci: (3± c,−1); (note: very close to the vertices!)

asymptotes: y + 1 = ±(1/32

)(x− 3)

5 10

-2

-1

Page 4: Warm up - City University of New York

36y2 − x2 + 72y + 6x+ 31 = 0: Hyperbola!

0 = 36y2−x2 + 72y + 6x+ 31

= 36(y2 + 2y)− (x2 − 6x) + 31

= 36((y + 1)2 − 1)− ((x− 3)2 − 9) + 31

= 36(y + 1)2 − (x− 3)2 + 4.

So 4 = (x− 3)2 − 36(y + 1)2. So

1 = (x− 3)2/4− 9(y + 1)2 =(x−32

)2 − (y+11/3

)2.

center: (3,−1); a = 2, b = 1/3,c =

√22 + (1/3)2 =

√37/3 ≈ 2.03; ;

vertices: (3± 2,−1);foci: (3± c,−1); (note: very close to the vertices!)

asymptotes: y + 1 = ±(1/32

)(x− 3)

5 10

-2

-1

Page 5: Warm up - City University of New York

36y2 − x2 + 72y + 6x+ 31 = 0: Hyperbola!

0 = 36y2−x2 + 72y + 6x+ 31

= 36(y2 + 2y)− (x2 − 6x) + 31

= 36((y + 1)2 − 1)− ((x− 3)2 − 9) + 31

= 36(y + 1)2 − (x− 3)2 + 4.

So 4 = (x− 3)2 − 36(y + 1)2. So

1 = (x− 3)2/4− 9(y + 1)2 =(x−32

)2 − (y+11/3

)2.

center: (3,−1); a = 2, b = 1/3,c =

√22 + (1/3)2 =

√37/3 ≈ 2.03; ;

vertices: (3± 2,−1);foci: (3± c,−1); (note: very close to the vertices!)

asymptotes: y + 1 = ±(1/32

)(x− 3)

5 10

-2

-1

Page 6: Warm up - City University of New York

36y2 − x2 + 72y + 6x+ 31 = 0: Hyperbola!

0 = 36y2−x2 + 72y + 6x+ 31

= 36(y2 + 2y)− (x2 − 6x) + 31

= 36((y + 1)2 − 1)− ((x− 3)2 − 9) + 31

= 36(y + 1)2 − (x− 3)2 + 4.

So 4 = (x− 3)2 − 36(y + 1)2. So

1 = (x− 3)2/4− 9(y + 1)2 =(x−32

)2 − (y+11/3

)2.

center: (3,−1); a = 2, b = 1/3,c =

√22 + (1/3)2 =

√37/3 ≈ 2.03; ;

vertices: (3± 2,−1);foci: (3± c,−1); (note: very close to the vertices!)

asymptotes: y + 1 = ±(1/32

)(x− 3)

5 10

-2

-1

Page 7: Warm up - City University of New York

y2 − 10y−8x+ 49 = 0: Sideways parabola! (opens to the right)

0 = y2−10y−8x+49 = (y−5)2−25−8x+49 = (y−5)2−8x+24,

so(y − 5)2 = 8x− 24 = 8(x− 3) = 4(2)(x− 3).

vertex: (3, 5); p = 2; focus: (3 + p, 5); directrix: x = 3− p

5

5

10

Page 8: Warm up - City University of New York

y2 − 10y−8x+ 49 = 0: Sideways parabola! (opens to the right)

0 = y2−10y−8x+49 = (y−5)2−25−8x+49 = (y−5)2−8x+24,

so(y − 5)2 = 8x− 24 = 8(x− 3) = 4(2)(x− 3).

vertex: (3, 5); p = 2; focus: (3 + p, 5); directrix: x = 3− p

5

5

10

Page 9: Warm up - City University of New York

y2 − 10y−8x+ 49 = 0: Sideways parabola! (opens to the right)

0 = y2−10y−8x+49 = (y−5)2−25−8x+49 = (y−5)2−8x+24,

so(y − 5)2 = 8x− 24 = 8(x− 3) = 4(2)(x− 3).

vertex: (3, 5); p = 2; focus: (3 + p, 5); directrix: x = 3− p

5

5

10

Page 10: Warm up - City University of New York

y2 + 2x2 + 4y + 8x+ 11 = 0: Ellipse!

0 = y2 + 2x2 + 4y + 8x+ 11

= (y2 + 4y) + 2(x2 + 4x) + 11

= ((y + 2)2 − 4) + 2((x+ 2)2 − 4) + 11

= (y + 2)2 + 2(x+ 2)2 − 1.

So

1 = (y + 2)2 + 2(x+ 2)2 = (y + 2)2 +

(x+ 2

1/√2

)2

.

center: (−2,−2);a = 1, b = 1/

√2,

c =√

12 − (1/√2)2 = 1/

√2 ≈ 0.71;

vertices: (−2,−2± a);foci: (−2,−2± c);major axis: x = −2

-3 -2 -1

-3

-2

-1

Page 11: Warm up - City University of New York

y2 + 2x2 + 4y + 8x+ 11 = 0: Ellipse!

0 = y2 + 2x2 + 4y + 8x+ 11

= (y2 + 4y) + 2(x2 + 4x) + 11

= ((y + 2)2 − 4) + 2((x+ 2)2 − 4) + 11

= (y + 2)2 + 2(x+ 2)2 − 1.

So

1 = (y + 2)2 + 2(x+ 2)2 = (y + 2)2 +

(x+ 2

1/√2

)2

.

center: (−2,−2);a = 1, b = 1/

√2,

c =√

12 − (1/√2)2 = 1/

√2 ≈ 0.71;

vertices: (−2,−2± a);foci: (−2,−2± c);major axis: x = −2

-3 -2 -1

-3

-2

-1

Page 12: Warm up - City University of New York

y2 + 2x2 + 4y + 8x+ 11 = 0: Ellipse!

0 = y2 + 2x2 + 4y + 8x+ 11

= (y2 + 4y) + 2(x2 + 4x) + 11

= ((y + 2)2 − 4) + 2((x+ 2)2 − 4) + 11

= (y + 2)2 + 2(x+ 2)2 − 1.

So

1 = (y + 2)2 + 2(x+ 2)2 = (y + 2)2 +

(x+ 2

1/√2

)2

.

center: (−2,−2);a = 1, b = 1/

√2,

c =√12 − (1/

√2)2 = 1/

√2 ≈ 0.71;

vertices: (−2,−2± a);foci: (−2,−2± c);major axis: x = −2

-3 -2 -1

-3

-2

-1

Page 13: Warm up - City University of New York

y2 + 2x2 + 4y + 8x+ 11 = 0: Ellipse!

0 = y2 + 2x2 + 4y + 8x+ 11

= (y2 + 4y) + 2(x2 + 4x) + 11

= ((y + 2)2 − 4) + 2((x+ 2)2 − 4) + 11

= (y + 2)2 + 2(x+ 2)2 − 1.

So

1 = (y + 2)2 + 2(x+ 2)2 = (y + 2)2 +

(x+ 2

1/√2

)2

.

center: (−2,−2);a = 1, b = 1/

√2,

c =√12 − (1/

√2)2 = 1/

√2 ≈ 0.71;

vertices: (−2,−2± a);foci: (−2,−2± c);major axis: x = −2

-3 -2 -1

-3

-2

-1

Page 14: Warm up - City University of New York

Conics with cross-terms

Again, all conic sections satisfy an equation of the form

Ax2 +Bxy + Cy2 +Dx+ Ey + F = 0

for some constants A,B,C,D,E, F .

Last time, we talked about how to analyze anything where B = 0.

Just like we can shift up/down or left/right to get from somethinglike

(y − 5)2 = 8(x− 3) to (y)2 = 8x,

we can rotate to get from something where B 6= 0 to somethingwhere B = 0.

Page 15: Warm up - City University of New York

Conics with cross-terms

Again, all conic sections satisfy an equation of the form

Ax2 +Bxy + Cy2 +Dx+ Ey + F = 0

for some constants A,B,C,D,E, F .

Last time, we talked about how to analyze anything where B = 0.

Just like we can shift up/down or left/right to get from somethinglike

(y − 5)2 = 8(x− 3) to (y)2 = 8x,

we can rotate to get from something where B 6= 0 to somethingwhere B = 0.

Page 16: Warm up - City University of New York

Conics with cross-terms

Again, all conic sections satisfy an equation of the form

Ax2 +Bxy + Cy2 +Dx+ Ey + F = 0

for some constants A,B,C,D,E, F .

Last time, we talked about how to analyze anything where B = 0.

Just like we can shift up/down or left/right to get from somethinglike

(y − 5)2 = 8(x− 3) to (y)2 = 8x,

we can rotate to get from something where B 6= 0 to somethingwhere B = 0.

Page 17: Warm up - City University of New York

Take the usual x, y-axis

, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

We want to take a point (x, y) and write it in terms of x and y.Easier to do in polar!In the x, y-frame,

x = r cos(φ) y = r sin(φ).But in the x, y-frame, the angle is φ+ θ, and the radius is thesame! So in the x, y-frame,

x = r cos(φ+ θ) y = r sin(φ+ θ).Now, using the angle addition formulas,

x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 18: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

We want to take a point (x, y) and write it in terms of x and y.Easier to do in polar!In the x, y-frame,

x = r cos(φ) y = r sin(φ).But in the x, y-frame, the angle is φ+ θ, and the radius is thesame! So in the x, y-frame,

x = r cos(φ+ θ) y = r sin(φ+ θ).Now, using the angle addition formulas,

x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 19: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

We want to take a point (x, y) and write it in terms of x and y.

Easier to do in polar!In the x, y-frame,

x = r cos(φ) y = r sin(φ).But in the x, y-frame, the angle is φ+ θ, and the radius is thesame! So in the x, y-frame,

x = r cos(φ+ θ) y = r sin(φ+ θ).Now, using the angle addition formulas,

x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 20: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

We want to take a point (x, y) and write it in terms of x and y.Easier to do in polar!

In the x, y-frame,x = r cos(φ) y = r sin(φ).

But in the x, y-frame, the angle is φ+ θ, and the radius is thesame! So in the x, y-frame,

x = r cos(φ+ θ) y = r sin(φ+ θ).Now, using the angle addition formulas,

x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 21: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

We want to take a point (x, y) and write it in terms of x and y.Easier to do in polar!In the x, y-frame,

x = r cos(φ) y = r sin(φ).

But in the x, y-frame, the angle is φ+ θ, and the radius is thesame! So in the x, y-frame,

x = r cos(φ+ θ) y = r sin(φ+ θ).Now, using the angle addition formulas,

x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 22: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

We want to take a point (x, y) and write it in terms of x and y.Easier to do in polar!In the x, y-frame,

x = r cos(φ) y = r sin(φ).But in the x, y-frame, the angle is φ+ θ, and the radius is thesame!

So in the x, y-frame,x = r cos(φ+ θ) y = r sin(φ+ θ).

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 23: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

We want to take a point (x, y) and write it in terms of x and y.Easier to do in polar!In the x, y-frame,

x = r cos(φ) y = r sin(φ).But in the x, y-frame, the angle is φ+ θ, and the radius is thesame! So in the x, y-frame,

x = r cos(φ+ θ) y = r sin(φ+ θ).

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 24: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

x = r cos(φ),y = r sin(φ)

x = r cos(φ+ θ)y = r sin(φ+ θ)

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ)

= x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 25: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

x = r cos(φ),y = r sin(φ)

x = r cos(φ+ θ)y = r sin(φ+ θ)

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),

y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).Combining these equations, we get

x cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 26: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

x = r cos(φ),y = r sin(φ)

x = r cos(φ+ θ)y = r sin(φ+ θ)

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ)

= x sin(θ) + y cos(θ).Combining these equations, we get

x cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 27: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

x = r cos(φ),y = r sin(φ)

x = r cos(φ+ θ)y = r sin(φ+ θ)

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 28: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

x = r cos(φ),y = r sin(φ)

x = r cos(φ+ θ)y = r sin(φ+ θ)

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0

= x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 29: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

x = r cos(φ),y = r sin(φ)

x = r cos(φ+ θ)y = r sin(φ+ θ)

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ))

= y.

Page 30: Warm up - City University of New York

Take the usual x, y-axis, and rotate it by θ in [0, π/2)to get a new x, y-axis:

x

y

x

y

θ

(x, y)

r φ

x = r cos(φ),y = r sin(φ)

x = r cos(φ+ θ)y = r sin(φ+ θ)

Now, using the angle addition formulas,x = r cos(φ+ θ) = r cos(φ) cos(θ)− r sin(φ) sin(θ) = x cos(θ)− y sin(θ),y = r sin(φ+ θ) = r cos(φ) sin(θ) + r sin(φ) cos(θ) = x sin(θ) + y cos(θ).

Combining these equations, we getx cos(θ) + y sin(θ) = x(cos2(θ) + sin2(θ)) + y · 0 = x, and−x sin(θ) + y cos(θ) = x · 0 + y(sin2(θ) + cos2(θ)) = y.

Page 31: Warm up - City University of New York

Change of coordinates for rotating axes:

x

y

x

y

θ

(x, y) = (x, y)

If I rotate the x, y-axis by θ to get new coordinates (x, y), then theconversion between coordinate systems is given by

x = x cos(θ)− y sin(θ) and y = x sin(θ) + y cos(θ)

x = x cos(θ) + y sin(θ) and y = −x sin(θ) + y cos(θ)

Page 32: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 33: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4)

=√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 34: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y)

, and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 35: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4)

=√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 36: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 37: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy

=(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 38: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)

= 12(x

2−y2) =(

x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 39: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2)

=(

x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 40: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 41: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x.

Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 42: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0

, which is equivalent to x = 0, andy = −x is equivalent to x+ y = 0, is equivalent to y = 0.

Also, in the x, y frame, the foci are (x, y) = (±2, 0). Sox = ±2 cos(π/4) + 0 · sin(π/4) = ±

√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 43: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0

, andy = −x is equivalent to x+ y = 0, is equivalent to y = 0.

Also, in the x, y frame, the foci are (x, y) = (±2, 0). Sox = ±2 cos(π/4) + 0 · sin(π/4) = ±

√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 44: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0

, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 45: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0).

Sox = ±2 cos(π/4) + 0 · sin(π/4) = ±

√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 46: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4)

= ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 47: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2

, andy = ±(2) sin(π/4) + 0 · cos(π/4) = ±

√2.

Page 48: Warm up - City University of New York

Example

Show that the function xy = 1 is a hyperbola rotated by π/4.What are the foci and the asymptotes?

Solution. Convert coordinates, using θ = π/4:

x = x cos(π/4)− y sin(π/4) =√22 (x− y), and

y = x sin(π/4) + y cos(π/4) =√22 (x+ y).

So, subbing into xy = 1, we get

1 = xy =(√

22 (x− y)

)(√22 (x+ y)

)= 1

2(x2−y2) =

(x√2

)2−(

y√2

)2.

In the x, y frame, the asymptotes are y = ±x. Buty = x is equivalent to x− y = 0, which is equivalent to x = 0, and

y = −x is equivalent to x+ y = 0, is equivalent to y = 0.Also, in the x, y frame, the foci are (x, y) = (±2, 0). So

x = ±2 cos(π/4) + 0 · sin(π/4) = ±√2, and

y = ±(2) sin(π/4) + 0 · cos(π/4) = ±√2.

Page 49: Warm up - City University of New York

Graphing xy = 1:

In summary, the function xy = 1 is the function(

x√2

)2−(

y√2

)2rotated by θ = π/4. In the x, y-frame, the asymptotes are x = 0and y = 0. The foci are (

√2,√2) and (−

√2,−√2).

^𝑥

^𝑦

𝑥

𝑦

(Compare to y = 1/x!)

Page 50: Warm up - City University of New York

Graphing xy = 1:

In summary, the function xy = 1 is the function(

x√2

)2−(

y√2

)2rotated by θ = π/4. In the x, y-frame, the asymptotes are x = 0and y = 0. The foci are (

√2,√2) and (−

√2,−√2).

^𝑥

^𝑦

𝑥

𝑦

(Compare to y = 1/x!)

Page 51: Warm up - City University of New York

Graphing xy = 1:

In summary, the function xy = 1 is the function(

x√2

)2−(

y√2

)2rotated by θ = π/4. In the x, y-frame, the asymptotes are x = 0and y = 0. The foci are (

√2,√2) and (−

√2,−√2).

^𝑥

^𝑦

𝑥

𝑦

(Compare to y = 1/x!)

Page 52: Warm up - City University of New York

Hypothesis: for a conic sectionAx2 +Bxy + Cy2 +Dx+ Ey + F = 0, there is some rotationalchange of coordinates in which the xy term is missing.

In the previous example, we were explicitly given the right angle torotate by to eliminate the xy-term.

Big question: How could we find this in general?

Strategy:Take a generic θ and plug the change of coordinates

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

in to the generic conic section equation.Collect “like terms” in x and y.The coefficient of xy will be in terms of θ, A, B, etc.. Solve for θso that, in this new equation, the coefficient of xy is 0.

Page 53: Warm up - City University of New York

Hypothesis: for a conic sectionAx2 +Bxy + Cy2 +Dx+ Ey + F = 0, there is some rotationalchange of coordinates in which the xy term is missing.

In the previous example, we were explicitly given the right angle torotate by to eliminate the xy-term.

Big question: How could we find this in general?

Strategy:Take a generic θ and plug the change of coordinates

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

in to the generic conic section equation.Collect “like terms” in x and y.The coefficient of xy will be in terms of θ, A, B, etc.. Solve for θso that, in this new equation, the coefficient of xy is 0.

Page 54: Warm up - City University of New York

Hypothesis: for a conic sectionAx2 +Bxy + Cy2 +Dx+ Ey + F = 0, there is some rotationalchange of coordinates in which the xy term is missing.

In the previous example, we were explicitly given the right angle torotate by to eliminate the xy-term.

Big question: How could we find this in general?

Strategy:Take a generic θ and plug the change of coordinates

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

in to the generic conic section equation.Collect “like terms” in x and y.The coefficient of xy will be in terms of θ, A, B, etc.. Solve for θso that, in this new equation, the coefficient of xy is 0.

Page 55: Warm up - City University of New York

Hypothesis: for a conic sectionAx2 +Bxy + Cy2 +Dx+ Ey + F = 0, there is some rotationalchange of coordinates in which the xy term is missing.

In the previous example, we were explicitly given the right angle torotate by to eliminate the xy-term.

Big question: How could we find this in general?

Strategy:Take a generic θ and plug the change of coordinates

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

in to the generic conic section equation.

Collect “like terms” in x and y.The coefficient of xy will be in terms of θ, A, B, etc.. Solve for θso that, in this new equation, the coefficient of xy is 0.

Page 56: Warm up - City University of New York

Hypothesis: for a conic sectionAx2 +Bxy + Cy2 +Dx+ Ey + F = 0, there is some rotationalchange of coordinates in which the xy term is missing.

In the previous example, we were explicitly given the right angle torotate by to eliminate the xy-term.

Big question: How could we find this in general?

Strategy:Take a generic θ and plug the change of coordinates

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

in to the generic conic section equation.Collect “like terms” in x and y.

The coefficient of xy will be in terms of θ, A, B, etc.. Solve for θso that, in this new equation, the coefficient of xy is 0.

Page 57: Warm up - City University of New York

Hypothesis: for a conic sectionAx2 +Bxy + Cy2 +Dx+ Ey + F = 0, there is some rotationalchange of coordinates in which the xy term is missing.

In the previous example, we were explicitly given the right angle torotate by to eliminate the xy-term.

Big question: How could we find this in general?

Strategy:Take a generic θ and plug the change of coordinates

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

in to the generic conic section equation.Collect “like terms” in x and y.The coefficient of xy will be in terms of θ, A, B, etc.. Solve for θso that, in this new equation, the coefficient of xy is 0.

Page 58: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 59: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:

−A cos(θ) sin(θ)−A sin(θ) cos(θ)+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 60: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)

−A sin(θ) cos(θ)+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 61: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 62: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)

−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 63: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)

+C sin(θ) cos(θ) + C cos(θ) sin(θ)= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 64: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ)

+ C cos(θ) sin(θ)= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 65: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 66: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))

= B cos(2θ) + (C −A) sin(2θ).So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 67: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 68: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0

, i.e. tan(2θ) = B/(A− C) .

Page 69: Warm up - City University of New York

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

= A(x cos(θ)− y sin(θ))(x cos(θ)− y sin(θ))+B(x cos(θ)− y sin(θ))(x sin(θ) + y cos(θ))

+ C(x sin(θ) + y cos(θ))(x sin(θ) + y cos(θ))

+D(x cos(θ)− y sin(θ)) + E(x sin(θ) + y cos(θ)) + F

Coefficient of xy:−A cos(θ) sin(θ)−A sin(θ) cos(θ)

+B cos(θ) cos(θ)−B sin(θ) sin(θ)+C sin(θ) cos(θ) + C cos(θ) sin(θ)

= B(cos2(θ)− sin2(θ)) + (C −A)(2 cos(θ) sin(θ))= B cos(2θ) + (C −A) sin(2θ).

So we want θ such that

B cos(2θ) + (C −A) sin(2θ) = 0, i.e. tan(2θ) = B/(A− C) .

Page 70: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

Rotating by θ eliminates the xy terms whentan(2θ) = B/(A− C).

What θ do you want to rotate by to graph each of the followingconic sections?Example: 8x2 − 4xy + 4y2 + 1 = 0.Solution: A = 8, B = −4, C = 4, so tan(2θ) = 4/(8− 4) = 1. So2θ = π/4. So θ = π/8.You try:

1. x2 − xy + y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 71: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

Rotating by θ eliminates the xy terms whentan(2θ) = B/(A− C).

What θ do you want to rotate by to graph each of the followingconic sections?

Example: 8x2 − 4xy + 4y2 + 1 = 0.Solution: A = 8, B = −4, C = 4, so tan(2θ) = 4/(8− 4) = 1. So2θ = π/4. So θ = π/8.You try:

1. x2 − xy + y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 72: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

Rotating by θ eliminates the xy terms whentan(2θ) = B/(A− C).

What θ do you want to rotate by to graph each of the followingconic sections?Example: 8x2 − 4xy + 4y2 + 1 = 0.

Solution: A = 8, B = −4, C = 4, so tan(2θ) = 4/(8− 4) = 1. So2θ = π/4. So θ = π/8.You try:

1. x2 − xy + y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 73: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

Rotating by θ eliminates the xy terms whentan(2θ) = B/(A− C).

What θ do you want to rotate by to graph each of the followingconic sections?Example: 8x2 − 4xy + 4y2 + 1 = 0.Solution: A = 8, B = −4, C = 4

, so tan(2θ) = 4/(8− 4) = 1. So2θ = π/4. So θ = π/8.You try:

1. x2 − xy + y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 74: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

Rotating by θ eliminates the xy terms whentan(2θ) = B/(A− C).

What θ do you want to rotate by to graph each of the followingconic sections?Example: 8x2 − 4xy + 4y2 + 1 = 0.Solution: A = 8, B = −4, C = 4, so tan(2θ) = 4/(8− 4) = 1.

So2θ = π/4. So θ = π/8.You try:

1. x2 − xy + y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 75: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

Rotating by θ eliminates the xy terms whentan(2θ) = B/(A− C).

What θ do you want to rotate by to graph each of the followingconic sections?Example: 8x2 − 4xy + 4y2 + 1 = 0.Solution: A = 8, B = −4, C = 4, so tan(2θ) = 4/(8− 4) = 1. So2θ = π/4. So θ = π/8.

You try:

1. x2 − xy + y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 76: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

Rotating by θ eliminates the xy terms whentan(2θ) = B/(A− C).

What θ do you want to rotate by to graph each of the followingconic sections?Example: 8x2 − 4xy + 4y2 + 1 = 0.Solution: A = 8, B = −4, C = 4, so tan(2θ) = 4/(8− 4) = 1. So2θ = π/4. So θ = π/8.You try:

1. x2 − xy + y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 77: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator. Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 78: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator.

Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 79: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator. Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 80: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator. Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 81: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator. Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 82: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator. Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 83: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator. Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 84: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)−y sin(θ), y = x sin(θ)+y cos(θ), tan(2θ) = B/(A−C).

Of course, plugging in things like θ = π/8 into sin(θ) and cos(θ)isn’t fun without a calculator. Draw a triangle for cos(2θ) and usethe half angle formulas!

cos2(θ) = 12(1 + cos(2θ)) sin2(θ) = 1

2(1− cos(2θ))

Example: If tan(2θ) = 1, then 2θ is the angle of the triangle

1

1c

c =√12 + 12 =

√2

cos(2θ) = 1/√2 =√2/2

cos(θ) =√

12(1 +

√2/2)

sin(θ) =√

12(1−

√2/2)

So

x = x√

12 (1 +

√22 )−y

√12 (1−

√22 ), y = x

√12 (1−

√22 )+y

√12 (1 +

√22 )

Page 85: Warm up - City University of New York

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

x = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ)

tan(2θ) = B/(A− C).cos2(θ) = 1

2(1 + cos(2θ)) sin2(θ) = 12(1− cos(2θ))

You try: Find the change of coordinates that will eliminate the xyterm in each of the following conic sections.

1. x2 − xy − y2 − 2 = 02. 4x2 − 4xy + 7y2 − 24 = 03. 2x2 + 4

√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 86: Warm up - City University of New York

Identifying the conic section

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

In the case we did last time, where B = 0, we identified the casesshape condition if B = 0:

parabola A = 0 or C = 0

AC = 0

ellipse A and C same signs

AC > 0

hyperbola A and C different signs

AC < 0Just like we did for calculating the coefficient of xy after changingcoordinates, we could calculate all the other coefficients after achange in coordinates

0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F.If we did, we could also show that the discriminants before andafter the change are the same, i.e.

B2 − 4AC = (B)2 − 4AC.But if we chose θ so that B = 0 (like we’ve been doing), then weget

B2 − 4AC = −4AC.

Page 87: Warm up - City University of New York

Identifying the conic section

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

In the case we did last time, where B = 0, we identified the casesshape condition if B = 0:

parabola A = 0 or C = 0 AC = 0ellipse A and C same signs AC > 0

hyperbola A and C different signs AC < 0Just like we did for calculating the coefficient of xy after changingcoordinates, we could calculate all the other coefficients after achange in coordinates

0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F.

If we did, we could also show that the discriminants before andafter the change are the same, i.e.

B2 − 4AC = (B)2 − 4AC.But if we chose θ so that B = 0 (like we’ve been doing), then weget

B2 − 4AC = −4AC.

Page 88: Warm up - City University of New York

Identifying the conic section

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

In the case we did last time, where B = 0, we identified the casesshape condition if B = 0:

parabola A = 0 or C = 0 AC = 0ellipse A and C same signs AC > 0

hyperbola A and C different signs AC < 0Just like we did for calculating the coefficient of xy after changingcoordinates, we could calculate all the other coefficients after achange in coordinates

0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F.If we did, we could also show that the discriminants before andafter the change are the same, i.e.

B2 − 4AC = (B)2 − 4AC.

But if we chose θ so that B = 0 (like we’ve been doing), then weget

B2 − 4AC = −4AC.

Page 89: Warm up - City University of New York

Identifying the conic section

0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

In the case we did last time, where B = 0, we identified the casesshape condition if B = 0:

parabola A = 0 or C = 0 AC = 0ellipse A and C same signs AC > 0

hyperbola A and C different signs AC < 0Just like we did for calculating the coefficient of xy after changingcoordinates, we could calculate all the other coefficients after achange in coordinates

0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F.If we did, we could also show that the discriminants before andafter the change are the same, i.e.

B2 − 4AC = (B)2 − 4AC.But if we chose θ so that B = 0 (like we’ve been doing), then weget

B2 − 4AC = −4AC.

Page 90: Warm up - City University of New York

Putting it together: we start with0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F,

and convert to0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F,

usingx = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ).

We choose θ such that B = 0, i.e. tan(2θ) = B/(A− C).Then since B2 − 4AC = (B)2 − 4AC, we get

−4AC = B2 − 4AC.

Using our table from before, we can classify the conic sectionaccording to the following table:

shape condition

parabola AC = 0

B2 − 4AC = 0

ellipse AC > 0

B2 − 4AC < 0

hyperbola AC < 0

B2 − 4AC > 0

Page 91: Warm up - City University of New York

Putting it together: we start with0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F,

and convert to0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F,

usingx = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ).

We choose θ such that B = 0, i.e. tan(2θ) = B/(A− C).

Then since B2 − 4AC = (B)2 − 4AC, we get

−4AC = B2 − 4AC.

Using our table from before, we can classify the conic sectionaccording to the following table:

shape condition

parabola AC = 0

B2 − 4AC = 0

ellipse AC > 0

B2 − 4AC < 0

hyperbola AC < 0

B2 − 4AC > 0

Page 92: Warm up - City University of New York

Putting it together: we start with0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F,

and convert to0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F,

usingx = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ).

We choose θ such that B = 0, i.e. tan(2θ) = B/(A− C).Then since B2 − 4AC = (B)2 − 4AC, we get

−4AC = B2 − 4AC.

Using our table from before, we can classify the conic sectionaccording to the following table:

shape condition

parabola AC = 0

B2 − 4AC = 0

ellipse AC > 0

B2 − 4AC < 0

hyperbola AC < 0

B2 − 4AC > 0

Page 93: Warm up - City University of New York

Putting it together: we start with0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F,

and convert to0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F,

usingx = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ).

We choose θ such that B = 0, i.e. tan(2θ) = B/(A− C).Then since B2 − 4AC = (B)2 − 4AC, we get

−4AC = B2 − 4AC.

Using our table from before, we can classify the conic sectionaccording to the following table:

shape condition

parabola AC = 0

B2 − 4AC = 0

ellipse AC > 0

B2 − 4AC < 0

hyperbola AC < 0

B2 − 4AC > 0

Page 94: Warm up - City University of New York

Putting it together: we start with0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F,

and convert to0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F,

usingx = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ).

We choose θ such that B = 0, i.e. tan(2θ) = B/(A− C).Then since B2 − 4AC = (B)2 − 4AC, we get

−4AC = B2 − 4AC.

Using our table from before, we can classify the conic sectionaccording to the following table:

shape condition

parabola AC = 0 B2 − 4AC = 0

ellipse AC > 0 B2 − 4AC < 0

hyperbola AC < 0 B2 − 4AC > 0

Page 95: Warm up - City University of New York

Putting it together: we start with0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F,

and convert to0 = A(x)2 +Bxy + C(y)2 +Dx+ Ey + F,

usingx = x cos(θ)− y sin(θ), y = x sin(θ) + y cos(θ).

We choose θ such that B = 0, i.e. tan(2θ) = B/(A− C).Then since B2 − 4AC = (B)2 − 4AC, we get

−4AC = B2 − 4AC.

Using our table from before, we can classify the conic sectionaccording to the following table:

shape condition

parabola AC = 0 B2 − 4AC = 0

ellipse AC > 0 B2 − 4AC < 0

hyperbola AC < 0 B2 − 4AC > 0

Page 96: Warm up - City University of New York

You try

Identify the kind of conic section given by each of the followingequations:

1. x2 − xy − y2 − 2 = 0

2. 4x2 − 4xy + 7y2 − 24 = 0

3. 2x2 + 4√3xy + 6y2 − 9x+ 9

√3y − 63 = 0

Page 97: Warm up - City University of New York

Graphing 0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

1. If B 6= 0, change coordinates using x = x cos(θ)− y sin(θ),y = x sin(θ) + y cos(θ), where tan(2θ) = B/(A− C).Tip: Use a triangle and the half-angle formulas to calculatecos(θ) and sin(θ).

2. With your new equation0 = A(x)2 + C(y)2 +Dx+ Ey + F,

get into one of the canonical forms and calculate all theimportant features of the graph.(If B = 0, then A = A, C = C, etc..)

3. Sketch the graph by first sketching the rotated axes and thengraphing theˆcurve on those axes.

4. If needed, convert features of the graph (like vertices, foci,asymptotes, etc.) back into x, y-coordinates using

x = x cos(θ) + y sin(θ) and y = −x sin(θ) + y cos(θ).

You try: Sketch a graph of 4x2 − 4xy + 7y2 − 24 = 0.

Page 98: Warm up - City University of New York

Graphing 0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

1. If B 6= 0, change coordinates using x = x cos(θ)− y sin(θ),y = x sin(θ) + y cos(θ), where tan(2θ) = B/(A− C).Tip: Use a triangle and the half-angle formulas to calculatecos(θ) and sin(θ).

2. With your new equation0 = A(x)2 + C(y)2 +Dx+ Ey + F,

get into one of the canonical forms and calculate all theimportant features of the graph.(If B = 0, then A = A, C = C, etc..)

3. Sketch the graph by first sketching the rotated axes and thengraphing theˆcurve on those axes.

4. If needed, convert features of the graph (like vertices, foci,asymptotes, etc.) back into x, y-coordinates using

x = x cos(θ) + y sin(θ) and y = −x sin(θ) + y cos(θ).

You try: Sketch a graph of 4x2 − 4xy + 7y2 − 24 = 0.

Page 99: Warm up - City University of New York

Graphing 0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

1. If B 6= 0, change coordinates using x = x cos(θ)− y sin(θ),y = x sin(θ) + y cos(θ), where tan(2θ) = B/(A− C).Tip: Use a triangle and the half-angle formulas to calculatecos(θ) and sin(θ).

2. With your new equation0 = A(x)2 + C(y)2 +Dx+ Ey + F,

get into one of the canonical forms and calculate all theimportant features of the graph.(If B = 0, then A = A, C = C, etc..)

3. Sketch the graph by first sketching the rotated axes and thengraphing theˆcurve on those axes.

4. If needed, convert features of the graph (like vertices, foci,asymptotes, etc.) back into x, y-coordinates using

x = x cos(θ) + y sin(θ) and y = −x sin(θ) + y cos(θ).

You try: Sketch a graph of 4x2 − 4xy + 7y2 − 24 = 0.

Page 100: Warm up - City University of New York

Graphing 0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

1. If B 6= 0, change coordinates using x = x cos(θ)− y sin(θ),y = x sin(θ) + y cos(θ), where tan(2θ) = B/(A− C).Tip: Use a triangle and the half-angle formulas to calculatecos(θ) and sin(θ).

2. With your new equation0 = A(x)2 + C(y)2 +Dx+ Ey + F,

get into one of the canonical forms and calculate all theimportant features of the graph.(If B = 0, then A = A, C = C, etc..)

3. Sketch the graph by first sketching the rotated axes and thengraphing theˆcurve on those axes.

4. If needed, convert features of the graph (like vertices, foci,asymptotes, etc.) back into x, y-coordinates using

x = x cos(θ) + y sin(θ) and y = −x sin(θ) + y cos(θ).

You try: Sketch a graph of 4x2 − 4xy + 7y2 − 24 = 0.

Page 101: Warm up - City University of New York

Graphing 0 = Ax2 +Bxy + Cy2 +Dx+ Ey + F

1. If B 6= 0, change coordinates using x = x cos(θ)− y sin(θ),y = x sin(θ) + y cos(θ), where tan(2θ) = B/(A− C).Tip: Use a triangle and the half-angle formulas to calculatecos(θ) and sin(θ).

2. With your new equation0 = A(x)2 + C(y)2 +Dx+ Ey + F,

get into one of the canonical forms and calculate all theimportant features of the graph.(If B = 0, then A = A, C = C, etc..)

3. Sketch the graph by first sketching the rotated axes and thengraphing theˆcurve on those axes.

4. If needed, convert features of the graph (like vertices, foci,asymptotes, etc.) back into x, y-coordinates using

x = x cos(θ) + y sin(θ) and y = −x sin(θ) + y cos(θ).

You try: Sketch a graph of 4x2 − 4xy + 7y2 − 24 = 0.

Page 102: Warm up - City University of New York